Yukawa位基态波函数的Green函数叠代求解

应用最近发展的沿一条确定的轨迹求解N维基态量子波函数的方法,首先由直接级数展开法得到Hulthen位的严格基态解和Yukawa位的近似基态解;并进一步运用Green函数叠代法及变分-叠代法求Yukawa位的基态近似解.     

强交换场中无隙超导电性的Eliashberg方程研究

本文研究强交换场中线性化的Eliashberg能隙方程。采用一个叠代方法考虑了能隙函数φ(ω)对±ω的不对称性。在叠代的最低阶给出了近似的解。所得的结果表明:对中等耦合强度以上(λ≥0.5)的电声子系统,能隙函数的不对称效应会显著影响临界交换场的数值。 关键词：     

薄膜椭偏测量的自适应混合反演算法

基于梯度的线性反演方法计算效率高,基于随机扰动的模拟退火方法寻找最优解能力强针对薄膜椭偏测量的多极值问题,综合两者的优点,提出一种求解薄膜椭偏测量问题的混合反演算法.模型每次扰动采用线性寻优方法搜寻局部最优解,叠代过程中采用均匀设计的模拟退火方法随机搜寻模型,使该算法有跳出局部最优解的能力,可以在较少的叠代次数内搜寻到全局最优解,从而提高求解薄膜椭偏测量非线性反演方法的计算效率.对反演过程控制参数进行讨论,该算法具有自适应的特点.计算表明,该算法可有效求解薄膜椭偏测量的多极值问题.     

叠砖的平衡问题

利用矩阵，解叠砖平衡时的一个多元一次方程。     

一种自适应滤波中步长因子调节的算法

本文在研究时变信道的自适应匹配中,采用了多途信道的横向滤波器模型(MA模型),为求滤波器权系数应用的是最小均方误差滤波方法。在最小均方误差滤波中无论是采用最徒下降法(Steepst Descent Method),还是最小均方算法(LMS Algorithm),在叠代方程中都要引入步长因子μ.以往对μ的取值只推导出一个范围0<μ<1/λ_(max),λ_(max)为采集信号自相关矩阵的最大本征值,且在叠代过程中是一个常数。但究竞取多大值?取小了自适应叠代方程收敛慢,取大了误差能量函数产生振荡,甚至发散。为寻找一种快速收敛的自适应滤波方法,以适应信道的时变特性时发现,对叠代步长因子μ作自适应调节,会使收敛速度有明显提高。     

动力学不连续性导致的奇异排斥子

借助一类具有“映孔”的分段线性一维映象，阐明“映孔导致激发”是“不连续性导致奇异排斥子”出现的结果，此奇异排斥子使得叠代轨道经过映孔逃出原混沌吸引子，从而造成混沌吸引子的突然扩张，证明了叠代轨害原吸引子中的寿命的反比于逃兔速率，并解析地得到了平均寿命随控制参量的变化关系。     

动力学不连续性所导致的奇异排斥子

借助一类具有“映孔”的分段线性一维映象，阐明“映孔导致激发”是“不连续性导致奇异排斥子”出现的结果．此奇异排斥子使得叠代轨道经过映孔逃出原混沌吸引子，从而造成混沌吸引子的突然扩张．证明了叠代轨道在原吸引子中的寿命反比于逃逸速率，并解析地得到了平均寿命随控制参量的变化关系     

高斯叠代法研究相控阵非线性声场

相控阵在聚焦超声治疗应用中不可避免地受到非线性影响,提出了采用高斯叠代法计算相控阵的非线性声场。在该方法中,利用预设焦点参数并应用伪逆矩阵算法得到阵元的激励参数;然后将阵元近似拟合成一组高斯声束的叠加,通过高斯声束叠代计算非线性声场。数值计算中以64阵元一维相控阵为研究对象;线性条件下,高斯叠代法结果与菲涅耳积分结果的误差低于0.5%,验证了该方法的可行性;单焦点及双焦点模式的相控阵非线性声场结果表明非线性效应能提高焦点聚焦性能,并且非线性效应与激励声压及激励频率成正比。      

任意截面介质波导导模的叠代矩量法分析

本文提出用以计算任意截面介质波导色散关系的叠代矩量法,并给出用叠代矩量法计算椭圆介质波导、三角形波导、平切圆波导、蛋形截面波导等的传播特性的实例.计算结果与有限元法、点匹配法等精确数值计算结果符合很好.本方法简便易行,计算工作量较小.     

任意旋成面气动正命题的变域变分有限元解

一、前言 文献[1]、[2]给出了旋成面叶栅变分有限元法,但与其它解法相似,仍需用叠代法逐次逼近求得出气角,才能得到满足库塔条件的叶栅内流场。特别对离心叶栅,困难更大,处理欠妥即会出现无解。而且,迄今为止发表的叶栅解法都仅能近似求得栅后流线,影响了S_1、S_2叠代求解精度。 本文利用变域变分原理及有限元解法相结合,将沿叶栅后缘延伸至栅后区的两条     

Dark and kink soliton solutions of the generalized ZK–BBM equation by iterative scheme

The generalized ZK–BBM equation is solved using iterative scheme of the Adomian decomposition method (ADM) and variational iteration method (VIM). A dark and a kink soliton solutions of the generalized ZK–BBM equation are obtained under initial conditions. The convergence analysis of the ADM and VIM solution shows that these solutions are convergent. The comparison of the ADM and VIM solutions with the exact solution shows that the solutions of the generalized ZK–BBM equation by the iterative methods are almost exact. The absolute errors show that the accuracy and efficiency of the ADM and VIM depend on the problem and its domain. It is found that the iterative scheme of Adomian decomposition method and variational iteration method are quite efficient for the soliton solution of the generalized ZK–BBM equation.     

Formulation of Zeeman modulation as a signal filter

The Bloch equation containing a Zeeman modulation field is solved analytically by treating the Zeeman modulation frequency as a perturbation. The absorption and dispersion signals at both 0 degrees and 90 degrees modulation phase are obtained. The solutions are valid to first order in the modulation frequency, but are otherwise valid for any value of modulation amplitude or microwave amplitude. A first order treatment of modulation frequency is shown to be a valid approximation over a wide range of typical experimental EPR conditions. The solutions derived from the Bloch equation suggest that the effect of over-modulation on first and second harmonic EPR spectra can be formulated as a mathematical filter that smoothes and broadens the under-modulated signal. The only adjustable filter parameter is a width that is equivalent to the applied peak-to-peak modulation amplitude. The true spin-spin and spin-lattice relaxation rates are completely determined from the under-modulated spectrum. The filters derived from the analytic solutions of the Bloch equation in the linear limit of modulation frequency are tested against numerical solutions of the Bloch equation that are valid for any modulation frequency to show their applicability. The filters are further tested using experimental EPR spectra. Experimental under-modulated spectra are mathematically filtered and compared with the experimental over-modulated spectra. The application of modulation filters to STEPR spectra is explored and limitations are discussed.     

Statistical model of an atom in electron scattering calculations

The parameters describing scattering of electrons by atoms, which usually involve multiple integration of the atomic potentials, may be severely affected by the accuracy of these potentials. In the present work an iterative procedure is proposed providing a sequence of solutions of the Thomas-Fermi equation with increasing accuracy. Such a sequence makes it possible to establish the sensitivity of a given parameter to the accuracy of the atomic potential, and consequently to determine the accurate value of this parameter. Based on the present solutions, the differential scattering cross-sections for the Thomas-Fermi atom are calculated, and are found to deviate from the literature data.     

求解不可压Navier-Stokes方程的一种新方法

以方腔自然对流问题为例阐述了数值求解不可压Navier-Stokes方程的新方法．该方法将四阶紧致差分格式(FCDS)和具有并行性的交替组显(AGE)迭代方法相结合；兼顾了稳定性，计算精度及并行性能．针对不同的Raleigh数和Prandtl数，对方腔内稳态自然对流进行了数值模拟，并将数值结果同前人结果进行了比较．     

Floquet–Bloch solutions in a sawtooth photonic crystal

Band structure of a sawtooth photonic crystal for optical wave propagation along the axis of periodicity is investigated. Floquet–Bloch solutions are found and illustrated for the bandgaps, allowed bands, and bandedges of the crystal. Special attention is given to the cases where Floquet–Bloch solutions become periodic functions.     

Numerical method for hydrodynamic modulation equations describing Bloch oscillations in semiconductor superlattices

We present a finite difference method to solve a new type of nonlocal hydrodynamic equations that arise in the theory of spatially inhomogeneous Bloch oscillations in semiconductor superlattices. The hydrodynamic equations describe the evolution of the electron density, electric field and the complex amplitude of the Bloch oscillations for the electron current density and the mean energy density. These equations contain averages over the Bloch phase which are integrals of the unknown electric field and are derived by singular perturbation methods. Among the solutions of the hydrodynamic equations, at a 70 K lattice temperature, there are spatially inhomogeneous Bloch oscillations coexisting with moving electric field domains and Gunn-type oscillations of the current. At higher temperature (300 K) only Bloch oscillations remain. These novel solutions are found for restitution coefficients in a narrow interval below their critical values and disappear for larger values. We use an efficient numerical method based on an implicit second-order finite difference scheme for both the electric field equation (of drift-diffusion type) and the parabolic equation for the complex amplitude. Double integrals appearing in the nonlocal hydrodynamic equations are calculated by means of expansions in modified Bessel functions. We use numerical simulations to ascertain the convergence of the method. If the complex amplitude equation is solved using a first order scheme for restitution coefficients near their critical values, a spurious convection arises that annihilates the complex amplitude in the part of the superlattice that is closer to the cathode. This numerical artifact disappears if the space step is appropriately reduced or we use the second-order numerical scheme.     

Numerical solutions of the orbital equations for diatomic molecules

A basis of Hermite splines is used in conjunction with the collocation method to solve the orbital equations for diatomic molecules. Accurate solutions of the Hartree-Fock equations are obtained using iterative methods over most regions of space, while solving the equations by Gaussian elimination near the nuclear centres. In order to improve the speed and accuracy of our iterative scheme, a new self-adjoint form of the Hartree-Fock equation is derived. Using this new equation, our iterative subroutines solve the Hartree-Fock equations to one part in 10⁶. The Gaussian elimination routines are accurate to better than one part in 10⁸.     

Radiative Transport in a Periodic Structure

We derive radiative transport equations for solutions of a Schrödinger equation in a periodic structure with small random inhomogeneities. We use systematically the Wigner transform and the Bloch wave expansion. The streaming part of the radiative transport equations is determined entirely by the Bloch spectrum, and the scattering part by the random fluctuations.     

Bloch方程的解析解及其在水峰抑制和特形脉冲设计中的应用

用Laplace变换方法求出了Bloch方程在各种不同物理条件下的解析解,这些解析解物理图象清楚,便于分析,克服了数值解中的困难.解析解和相应的结论已用于水峰抑制和特形脉冲的设计.对于水峰抑制,本文指出抑制效果是有极限的,并给出了抑制效果的极限以及最佳抑制时间的近似计算公式.在特形脉冲的模拟过程中,我们发现只有同时考虑全部四类解析解,才能得到正确的模拟结果,另外,模拟还表明,要在保持激励频谱形状不变的条件下,得到不同倾倒角的脉冲必须改变激励脉冲的形状,相应实验的结果与我们给出的上述结论完全吻合。